Vertex function

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Template:Short description In quantum electrodynamics, the vertex function describes the coupling between a photon and an electron beyond the leading order of perturbation theory. In particular, it is the one particle irreducible correlation function involving the fermion <math>\psi</math>, the antifermion <math>\bar{\psi}</math>, and the vector potential A.

Definition

The vertex function <math>\Gamma^\mu</math> can be defined in terms of a functional derivative of the effective action Seff as

<math>\Gamma^\mu = -{1\over e}{\delta^3 S_{\mathrm{eff}}\over \delta \bar{\psi} \delta \psi \delta A_\mu}</math>
File:Vertex correction.svg
The one-loop correction to the vertex function. This is the dominant contribution to the anomalous magnetic moment of the electron.

The dominant (and classical) contribution to <math>\Gamma^\mu</math> is the gamma matrix <math>\gamma^\mu</math>, which explains the choice of the letter. The vertex function is constrained by the symmetries of quantum electrodynamics — Lorentz invariance; gauge invariance or the transversality of the photon, as expressed by the Ward identity; and invariance under parity — to take the following form:

<math> \Gamma^\mu = \gamma^\mu F_1(q^2) + \frac{i \sigma^{\mu\nu} q_{\nu}}{2 m} F_2(q^2) </math>

where <math> \sigma^{\mu\nu} = (i/2) [\gamma^{\mu}, \gamma^{\nu}] </math>, <math> q_{\nu} </math> is the incoming four-momentum of the external photon (on the right-hand side of the figure), and Template:Math and Template:Math are the Dirac and Pauli form factors,<ref>Template:Cite book</ref> respectively, that depend only on the momentum transfer q2. At tree level (or leading order), Template:Math and Template:Math. Beyond leading order, the corrections to Template:Math are exactly canceled by the field strength renormalization. The form factor Template:Math corresponds to the anomalous magnetic moment a of the fermion, defined in terms of the Landé g-factor as:

<math> a = \frac{g-2}{2} = F_2(0) </math>

In 1948, Julian Schwinger calculated the first correction to anomalous magnetic moment, given by

<math> F_2(0)\approx \frac{\alpha}{2\pi} </math>

where α is the fine-structure constant.<ref>Template:Cite journal</ref>

See also

References

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